RELATED APPLICATIONS
GOVERNMENT FUNDING
[0002] This invention was made with government support under Grant No. HR0011-11-C-0093
awarded by DARPA (Department of Defense). The government has certain rights in the
invention.
FIELD
[0003] The present invention generally relates to the manipulation of species using acoustic
waves such as surface acoustic waves.
BACKGROUND
[0004] Surface acoustic waves (SAWs) provide a method for driving flows and directing particle
motion, e.g., in microfluidic systems. The acoustic waves generated by a SAW transducer
can efficiently actuate broad classes of species including particles, beads, cells,
gels, and droplets in continuous flow. Devices based on acoustic waves can be used
to manipulate cells and particles. These devices feature control of each particle's
spatial position through dynamic patterning of the underlying acoustic standing wave.
However, most SAW sorters only utilize the component of the acoustic wave that is
oriented in the plane of the device, despite the fact that the acoustic wave's normal
component is several fold greater in magnitude. There has yet to be a SAW device which
takes advantage of the normal component of the acoustic wave for sorting purposes.
[0005] US 7,942,568 B1 relates to an active micromixer using a surface acoustic wave propagating on a piezoelectric
substrate to induce acoustic streaming in a fluid in a microfluidic channel.
[0006] US 2013/0192958 A1 relates to an apparatus for manipulating particles using tunable standing surface
acoustic waves, including a channel defined on a substrate and a pair of variable
frequency interdigital transducers.
SUMMARY
[0007] The present invention is defined by the independent claim 1. Preferred embodiments
are defined by the dependent claims. Further aspects are provided for facilitating
the understanding of the invention. The present invention generally relates to the
manipulation of species using acoustic waves such as surface acoustic waves. The subject
matter of the present invention involves, in some cases, interrelated products, alternative
solutions to a particular problem, and/or a plurality of different uses of one or
more systems and/or articles.
[0008] The following describes exemplary apparatus related to, but not part of, the claimed
invention.
[0009] In one set of examples, the apparatus comprises a microfluidic channel having a groove
defined in a first surface, the groove having a cross-sectional dimension sized to
allow a mammalian cell to fit within the groove, and an acoustic wave generator positioned
proximate a second surface of the microfluidic channel, the second surface adjacent
to the first surface.
[0010] The apparatus, in accordance with another set of examples , includes a microfluidic
channel having a groove defined in a first surface, the groove having a cross-sectional
dimension having a cross-sectional dimension of at least about 30 micrometers, and
an acoustic wave generator positioned proximate a second surface of the microfluidic
channel, the second surface adjacent to the first surface.
[0011] In still another set of examples , the apparatus comprises a microfluidic channel
having a first channel portion and a second channel portion, and a transducer positioned
to apply acoustic waves to the microfluidic channel. In some cases, the second channel
is positioned such that acoustic waves from the transducer can reach the second channel
portion without passing through the first channel portion and the first channel portion
without passing through the second channel portion. In certain instances, the second
channel is positioned such that acoustic waves from the transducer do not directly
pass through the second channel portion.
[0012] The apparatus, in yet another set of examples, comprises a microfluidic channel having
a first portion having a first outlet and a second portion having a second outlet.
In some cases, the first portion and the second portion are arranged orthogonally
with respect to a direction of average fluid flow within the channel. The apparatus
may also comprise a transducer positioned to apply acoustic waves to at least a portion
of the microfluidic channel. In some examples, the transducer is positioned to apply
acoustic waves in a direction substantially orthogonal to the direction of average
fluid flow within the channel, and/or substantially orthogonal to the arrangement
of the first portion and the second portion.
[0013] According to still another set of examples, the apparatus comprises a microfluidic
channel having a first portion containing a plurality of species flowing therethrough
and a second portion free of the species, and an acoustic wave generator positioned
to apply acoustic waves to at least a portion of the microfluidic channel to cause
at least some of the species to move from the first portion to the second portion
of the microfluidic channel. In some cases, an imaginary plane separating the first
portion and the second portion is not substantially orthogonal to the direction of
acoustic wave propagation from the transducer.
[0014] The present invention is directed to a sorting method, as defined in claim 1. The
method includes flowing a species contained in a fluid within a microfluidic channel
having a first outlet and a second outlet, and applying acoustic waves to deflect
the species to enter the second outlet, where in the absence of the acoustic waves,
the species enters the first outlet. The acoustic waves may be applied using an acoustic
wave generator to deflect the species within the microfluidic channel in a direction
having an axial component defined by propagation of the acoustic waves from the acoustic
wave generator and a lateral component defined substantially orthogonally thereto.
The lateral component is greater than the axial component.
[0015] Also described herein but not part of the claimed invention are methods of making
one or more of the microfluidic devices described herein for sorting cells, particles,
or other species. The present invention encompasses methods of using one or more of
the microfluidic devices described herein for sorting cells, particles, or other species.
[0016] Other advantages and novel features of the present invention will become apparent
from the following detailed description of various non-limiting embodiments of the
invention when considered in conjunction with the accompanying figures.
BRIEF DESCRIPTION OF THE DRAWINGS
[0017] Non-limiting embodiments of the present invention will be described by way of example
with reference to the accompanying figures, which are schematic and are not intended
to be drawn to scale. In the figures, each identical or nearly identical component
illustrated is typically represented by a single numeral. For purposes of clarity,
not every component is labeled in every figure, nor is every component of each embodiment
of the invention shown where illustration is not necessary to allow those of ordinary
skill in the art to understand the invention. In the figures:
Figs. 1A-1D schematically illustrate a device for sorting species;
Figs. 2A-2B illustrate a device for sorting cells, for use in the method of the invention;
Figs. 3A-3D illustrate characteristics of a sorting device, used in the method of
the invention;
Fig. 4 illustrates sorting purities, in still another embodiment of the invention;
Figs. 5A-5B illustrate variations in flow rate and groove width for devices in accordance
with still other embodiments of the invention;
Figs. 6A-6C illustrate operation of a device in yet another embodiment of the invention;
Fig. 7 illustrates a tapered interdigital transducer in accordance with another embodiment
of the invention; and
Figs. 8A-8C illustrate various devices according to yet other embodiments of the invention.
DETAILED DESCRIPTION
[0018] The present invention generally relates to the manipulation of species using acoustic
waves such as surface acoustic waves. In some aspects, a channel such as a microfluidic
channel may be provided having two or more outlets, and acoustic waves applied to
species within the channel to determine which outlet the species is directed to. For
instance, surface acoustic waves may be applied to a species such as a cell or a particle
to deflect it from the channel into a groove or other portion that directs it to a
different outlet. In some cases, surprisingly, this deflection of species may be in
a different direction than the incident acoustic waves on the channel. Other embodiments
of the present invention are generally directed to kits including such systems, techniques
for producing such systems, or the like.
[0019] One aspect of the invention is now described with reference to Fig. 6A as an illustrative,
non-limiting example. In this figure, a species 10, such as a cell or a particle,
is to be sorted or otherwise manipulated. Species 10 is contained in a fluid 15 within
a channel 20, such as a microfluidic channel. The fluid may be, for example, water
or another aqueous fluid, such as saline. In one set of embodiments, the species is
to be sorted to a first outlet 21 or a second outlet 22.
[0020] Normally, species 10 will flow through channel 20 from left to right, as indicated
by arrow 18, until it exits the channel through outlet 21 (e.g., to enter another
channel, a reactor, a collection chamber, etc.), as are indicated by dotted lines
in this figure. However, in some cases, acoustic waves 30 may be applied by transducer
35, or other acoustic wave generator. The transducer may be, for example, an interdigitated
transducer, such as a tapered interdigital transducer (see, e.g. Fig. 7). The transducer
may be positioned to apply acoustic waves at a side or surface 40 of the channel,
as is shown in Fig. 6A.
[0021] The acoustic waves can cause deflection of species 10 to facilitate sorting. For
instance, the acoustic waves can be applied when a certain species 10 is detected
or determined (for example, a fluorescence signal). Surprisingly, rather than being
simply deflected directly repulsively away from transducer 35, species 10 may be deflected
upwardly or at an angle away from transducer 35, relative to the position of transducer
35 and the propagation of acoustic waves from the transducer. The deflection can be
thought of as having two components: an axial component defined by the propagation
of the acoustic waves from the transducer, and a lateral component defined orthogonally
from the axial component, e.g., upward as shown in Fig. 1. Without wishing to be bound
by any theory, it is believed that under some conditions, refraction of acoustic waves
30 as the acoustic waves enter fluid 15 may cause the acoustic waves to change direction,
such that the waves do not merely propagate directly away from the transducer, but
instead propagates at an angle relative to its initial direction.
[0022] In some embodiments, this may be used to move species, e.g., that are contained in
fluid 15 within channel 20. Thus, for example, this may be used to move the species
into a second channel portion. In Fig. 6A, this channel portion is depicted as groove
50, and is positioned on a surface 45 adjacent to the surface to which the acoustic
waves are applied. Only a single groove 50 is present in this example. Groove 50 is
positioned at an angle towards outlet 22. However, in other embodiments, other configurations
for the second channel are also possible, and the deflection need not necessarily
be upward ("upward" is shown in Fig. 6A merely for ease of presentation). In this
figure, species 10 can be moved into and contained within groove 50, and thereby directed
to outlet 22 rather than outlet 21. Accordingly, upon application of a suitable acoustic
wave, species 10 may be directed to groove 50 to outlet 22, rather than proceeding
through to outlet 21. In this way, a plurality of species may be sorted.
[0023] The above discussion is a non-limiting example of one embodiment of the present invention
that can be used to sort a species, such as a cell or a particle. However, other embodiments
are also possible.
[0024] For instance, in one aspect, the present invention is generally directed to the manipulation
of species in a channel using acoustic waves such as surface acoustic waves. The species
may be, for example, cells or particles, or other species as described herein, that
can be manipulated in some fashion (e.g., moved, repelled, deflected, etc.) using
acoustic waves. For example, the species may be moved from a first portion of a channel
to a second portion of the channel under the influence of the acoustic waves.
[0025] In one set of embodiments, acoustic waves are applied at a surface of a channel to
manipulate a species contained in a fluid within the channel. Surprisingly, the acoustic
waves may cause the species to move in a direction different from the direction of
propagation of acoustic waves reaching the channel. Without wishing to be bound by
any theory, it is believed that the acoustic waves may refract upon entering the fluid
(i.e., through the channel wall, thereby propagating in a different direction). The
angle at which the acoustic waves are diffracted may be governed by factors such as
the speed of sound in the fluid and in the channel walls. For instance, as is shown
in Fig. 6B, acoustic waves 30 entering fluid 15 through wall 33 may be refracted,
which may cause the movement or deflection of species 10 in a lateral direction (indicated
by arrow 61), rather than in an axial direction away from the direction of propagation
(indicated by arrow 62).
[0026] This deflection can be thought of as having two vector components: an axial component
70 as is shown in Fig. 6C (defined by the direction of propagation of acoustic waves),
and a lateral component 75 defined orthogonally to the axial component. The ratio
between the two of these vector components defines the angle of deflection. In some
cases, the lateral component is equal to or greater than the axial component, and
in some cases, the lateral component may be at least about 1.5, at least about 2,
at least about 2.5, at least about 3, at least about 4, at least about 5 times, at
least about 10 times, at least about 20 times, at least about 30 times, at least about
50 times, at least about 75 times, or at least about 100 times greater. In addition,
in other embodiments, the lateral component may be less than the axial component.
It should be noted that "upwardly" is used here merely for convenience and ease of
presentation only; in reality, the channel and the channel walls may be positioned
in any suitable orientation, not necessarily parallel to the ground. Also, in some
cases, the deflection may be "down" instead of "up."
[0027] In one set of embodiments, one or more species may be present in a first channel
portion but not in a second channel portion. For example, an obstruction or other
obstacle may be used to divert species to a first channel portion, such as is shown
in Fig. 8A; as another non-limiting example, a species may simply be inserted into
the fluid in the first channel portion but not the second channel portion. By applying
suitable acoustic waves, the species in the first channel portion may be diverted
to a second channel portion, for example, a groove as is shown in Fig. 8A. In some
cases, the acoustic waves may be applied only at the first channel portion, or pass
through both portions such that the acoustic waves reaching the second channel portion
do not pass through the first channel portion. In some embodiments, the second channel
portion may be positioned such that at least part of the second channel portion is
positioned laterally with respect to the first channel portion, relative to the direction
of acoustic wave propagation. Optionally, the first portion and the second portion
may be separated by an imaginary plane, which may be positioned such that it is not
substantially orthogonal to the direction of acoustic wave propagation.
[0028] The second channel portion may be present on or be defined by a surface of a channel.
The second channel portion may be a groove, indentation, or other surface feature.
The second channel portion can have straight sides, curved sides, or the like. The
second channel portion may be shaped or sized to allow the species to enter in, and/or
to move the species to an outlet, i.e., a second outlet. In such a manner, one or
more species may be desirably directed to either a first outlet or a second outlet
based on application of an acoustic wave.
[0029] In one set of embodiments, the second channel portion may have the shape of a groove.
A non-limiting example is illustrated in Fig. 8A. The second channel portion may be
sized to have a cross-sectional dimension that allows the species to enter within
the second channel portion, e.g., to direct the species to an outlet. In addition,
in some cases, the second channel portion may be slanted or positioned, e.g., at a
nonzero angle with respect to the channel, to direct the species to the outlet. Any
suitable angle can be used, e.g., about 0°, about 5°, about 10°, about 20°, about
30°, about 40°, about 50°, about 60°, about 70°, about 80°, about 90°, about 100°,
about 110°, about 120°, about 130°, about 140°, about 150°, about 160°, about 170°,
about 175°, about 180° etc. Thus, as an example, the second channel portion may contain
at least one wall that is not parallel or perpendicular to the channel.
[0030] However, while a slanted groove is shown in Fig. 8A, it should be understood that
this is by way of example only. In other embodiments, the second channel portion may
have a variety of other shapes, such as those shown in Figs. 8B and 8C. In addition,
as mentioned, in some cases, three, four, or more outlets may be present, such as
is shown in Fig. 8D (top view) with outlets 21, 22, and 23. Sorting or manipulation
of one or more species may be controlled by one, or more than one, acoustic wave generator.
For instance, in some cases, a first acoustic wave may deflect a species to second
portion 50, while a second acoustic wave (from the same or different acoustic wave
generators) may deflect a species to third portion 53. By applying suitable acoustic
waves (or not applying an acoustic wave), a species may be directed into any desired
outlet.
[0031] As mentioned, the second channel portion may be sized to accept the entry of a species
therein, at least in certain embodiments. The second channel portion can have, for
example, a cross-sectional dimension (i.e., relative to average fluid flow within
the second channel portion) of at least about 10 micrometers, at least about 15 micrometers,
at least about 20 micrometers, at least about 25 micrometers, at least about 30 micrometers,
at least about 40 micrometers, at least about 50 micrometers, at least about 75 micrometers,
at least about 100 micrometers, at least about 150 micrometers, at least about 200
micrometers, at least about 250 micrometers, at least about 500 micrometers, etc.
In some cases, the second channel portion has a maximum cross-sectional dimension
that is less than the maximum cross-sectional dimension of the channel.
[0032] Thus, certain aspects of the present invention relate to the control or manipulation
of species, for example, in microfluidic systems. For instance, according to one set
of embodiments, species such as cells or particles may be sorted using acoustic waves.
The species may be any suitable species that can be manipulated by an applied acoustic
wave. Non-limiting examples include cells (for example, human cells, mammalian cells,
bacterial cells, etc.), particles, droplets, gels, bubbles, quantum dots, beads (e.g.,
fluorescent beads), viruses, or the like. In some cases, the species may contain other
entities therein (for example, nucleic acids such as siRNA, RNAi and DNA, proteins,
peptides, or enzymes, chemicals, polymers, drugs, etc.).
[0033] In some cases, for example, a species may be sorted or otherwise manipulated at relatively
high rates. For example, a characteristic of a species may be sensed and/or determined
in some fashion (e.g., as further described herein), then the species may be directed
towards a particular region of the device, such as a channel or an outlet, for example,
for sorting purposes.
[0034] In certain embodiments, a channel can include at least a first outlet and a second
outlet. In some cases, more than one inlet channel and/or more than one outlet channel
may be present. By suitable application of surface acoustic waves, droplets contained
within a fluid flowing through the channel may be directed into the first outlet or
the second outlet. In other embodiments, however, other configurations of channels
and junctions may be used, e.g., as described herein.
[0035] In some embodiments, species such as cells or particles may be sorted at relatively
high rates. For instance, at least about 10 species per second may be sorted in some
cases, and in other cases, at least about 20 species per second, at least about 30
species per second, at least about 100 species per second, at least about 200 species
per second, at least about 300 species per second, at least about 500 species per
second, at least about 750 species per second, at least about 1,000 species per second,
at least about 1,500 species per second, at least about 2,000 species per second,
at least about 3,000 species per second, at least about 5,000 species per second,
at least about 7,500 species per second, at least about 10,000 species per second,
at least about 15,000 species per second, at least about 20,000 species per second,
at least about 30,000 species per second, at least about 50,000 species per second,
at least about 75,000 species per second, at least about 100,000 species per second,
at least about 150,000 species per second, at least about 200,000 species per second,
at least about 300,000 species per second, at least about 500,000 species per second,
at least about 750,000 species per second, at least about 1,000,000 species per second,
at least about 1,500,000 species per second, at least about 2,000,000 or more species
per second, or at least about 3,000,000 or more species per second may be sorted or
otherwise manipulated. In some cases, as discussed, this control may be on a single
species basis, e.g., through the use of suitable acoustic waves.
[0036] In one aspect, the present invention is generally directed to applying acoustic waves,
such as surface acoustic waves, to a fluid containing species flowing in a channel,
such as a microfluidic channel. The acoustic waves may be applied by a suitable acoustic
wave generator. A surface acoustic wave ("SAW") is, generally speaking, an acoustic
wave able to travel along the surface of a material exhibiting elasticity, with an
amplitude that typically decays exponentially with depth into the material. By selecting
suitable acoustic waves, pressure changes may be induced in the fluid, which can be
used to manipulate the fluid in some cases. For example, acoustic waves applied to
a fluid may increase or decrease the pressure on the fluid, which may cause the fluid
to flow faster or slower due to the change in pressure, relative to fluid flow in
the absence of the acoustic waves. As other examples, the acoustic waves may be used
to deflect the fluid or to cause fluid to flow to a different location.
[0037] In some cases, the magnitude of the pressure change is related to the power or the
amplitude of the applied acoustic waves. In certain embodiments, the acoustic waves
may be applied at an amplitude and/or at a direction selected to alter a flow characteristic
of the fluid, e.g., its flow rate or direction of flow. Thus, for example, acoustic
waves may be used to sort species such as cells or particles, or other species discussed
herein.
[0038] The acoustic waves may be applied at varying amplitudes or powers in some cases.
In some cases, the pressure changes created in the fluid may be a function of the
power of the acoustic wave. For example, the acoustic waves may have a power of at
least about 0 dBm, at least about 3 dBm, at least about 6 dBm, at least about 9 dBm,
at least about 12 dBm, at least about 15 dBm, at least about 20 dBM, etc. The acoustic
waves may also have any suitable average frequency, in various embodiments. For example,
the average frequency of the acoustic waves may be between about 100 MHz and about
200 MHz, between about 130 MHz and about 160 MHz, between about 140 MHz and about
150 MHz, between about 100 MHz and about 120 MHz, between about 120 MHz and about
140 MHz, between about 140 MHz and about 160 MHz, between about 160 MHz and about
180 MHz, or between about 180 MHz and about 200 MHz or the like, and/or combinations
thereof. In other embodiments, the frequency may be between about 50 Hz and about
100 KHz, between about 100 Hz and about 2 kHz, between about 100 Hz and about 1,000
Hz, between about 1,000 Hz and about 10,000 Hz, between about 10,000 Hz and about
100,000 Hz, or the like, and/or combinations thereof. In some cases, the frequency
may be at least about 10 Hz, at least about 30 Hz, at least about 50 Hz, at least
about 100 Hz, at least about 300 Hz, at least about 1,000 Hz, at least about 3,000
Hz, at least about 10,000 Hz, at least about 30,000 Hz, at least about 100,000 Hz,
at least about 300,000 Hz, at least about 1 MHz, at least about 3 MHz, at least about
10 MHz, at least about 30 MHz, at least about 100 MHz, at least about 300 MHz, or
at least about 1 GHz or more in some embodiments. In certain instances, the frequency
may be no more than about 1 GHz, no more than about 300 MHz, no more than about 100
MHz, no more than about 30 MHz, no more than about 10 MHz, no more than about 3 MHz,
no more than about 1 MHz, no more than about 300,000 Hz, no more than about 100,000
Hz, no more than about 30,000 Hz, no more than about 10,000 Hz, no more than about
3,000 Hz, no more than about 1,000 Hz, no more than about 300 Hz, no more than about
100 Hz, or the like.
[0039] The acoustic waves may be applied, in some embodiments, in a downstream direction
or an upstream direction, relative to the flow of fluid in a channel, which can be
used to increase or decrease fluid flow within the channel. For example, acoustic
waves may be applied to a channel, such as a microfluidic channel, in a direction
of fluid flow within the channel, in a direction opposite of fluid flow within the
channel, or in another direction (e.g., perpendicular to fluid flow within the channel).
In other embodiments, the acoustic waves may be applied at any suitable angle relative
to the channel, for example, about 0°, about 5°, about 10°, about 20°, about 30°,
about 40°, about 50°, about 60°, about 70°, about 80°, about 90°, about 100°, about
110°, about 120°, about 130°, about 140°, about 150°, about 160°, about 170°, about
175°, about 180° etc.). It should be noted that in addition to this angle, there may
be a change in angle caused by refraction, as discussed herein.
[0040] In some cases, more than one acoustic wave may be applied to control fluid flow within
the channel, e.g., to sort species such as cells or particles. For example, a first
acoustic wave generator may be used to increase the pressure within the channel and
the second used to decrease the pressure within the channel (e.g., relative to the
pressure when no acoustic waves are present), the first acoustic wave generator may
be used to increase fluid flow and the second acoustic wave generator used to decrease
fluid flow, etc. (e.g., relative to the fluid flow when no acoustic waves are present).
The acoustic waves may be applied at the same, or different regions of a channel,
depending on the application. For instance, in some cases, a first acoustic wave and
a second acoustic wave may be applied to overlapping portions of a fluid, or a first
acoustic wave may be applied to a first portion of a fluid within a channel, and the
second acoustic wave may be applied to a second portion of the fluid within the channel.
If more than one acoustic wave is applied to a fluid, the acoustic waves may be applied
in any suitable order, e.g., simultaneously, sequentially, periodically, etc.
[0041] Without wishing to be bound by any theory, it should be noted that acoustic waves
may be very rapidly controlled, e.g., electrically, and typically can be applied to
fluids at very small time scales. Thus, individual regions of fluids (for example,
within a channel) may be controlled to an arbitrary degree, e.g., without affecting
other regions of fluids, even nearby or adjacent ones. Thus, for example, a single
species may be sorted independent of other species within the fluid. In some cases,
acoustic waves can be applied to a first region, then no acoustic waves may be applied,
or acoustic waves of a different magnitude and/or frequency, applied to an adjacent
or nearby second region. Thus, each region can be independently controlled, for instance,
for sorting purposes, without affecting adjacent or nearby regions.
[0042] In one set of embodiments, the characteristic response time, i.e., the time it takes
to see a change in a fluid region created by the presence of the acoustic wave, may
be smaller than the time it takes that fluid region to fully pass a specific location
within the channel, thereby allowing a high degree of control of the fluid region.
Thus, a single species, such as a cell or particle, may be controlled without affecting
other, nearby species. In contrast, many other systems or methods for controlling
fluids within a channel, such as a microfluidic channel, typically rely on fluid characteristics
or characteristics of the channel, which often have characteristic response times
that are much longer, e.g., such that individual droplets or regions cannot be independently
controlled.
[0043] In addition, in some cases, the acoustic waves may be applied continuously, or intermittently
or "pulsed." In addition, in some cases, the acoustic waves may be constant (i.e.,
having a fixed magnitude), or the acoustic waves may have an amplitude whose magnitude
varies in time, e.g., the acoustic waves may have an amplitude that varies independently
of the frequency of the acoustic waves.
[0044] As discussed, the acoustic waves may be applied to any suitable channel. In one set
of embodiments, the acoustic waves are applied to a fluid contained within a channel,
such as a microfluidic channel, to sort a species. Various examples of microfluidic
channels are discussed herein. More than one fluid may be present within the channel,
in some instances, e.g., flowing as separate phases (for example, side-by-side, as
droplets of a first fluid contained within a second fluid, etc.). Non-limiting examples
of such channels include straight channels, bent channels, droplet-making channel
configurations, and the like.
[0045] In addition, in some embodiments, the acoustic waves may be applied at similar modulation
frequencies, i.e., at least about 10 Hz, at least about 20 Hz, at least about 30 Hz,
at least about 100 Hz, at least about 200 Hz, at least about 300 Hz, at least about
500 Hz, at least about 750 Hz, at least about 1,000 Hz, at least about 1,500 Hz, at
least about 2,000 Hz, at least about 3,000 Hz, at least about 5,000 Hz, at least about
7,500 Hz, at least about 10,000 Hz, at least about 15,000 Hz, at least about 20,000
Hz, at least about 30,000 Hz, at least about 50,000 Hz, at least about 75,000 Hz,
at least about 100,000 Hz, at least about 150,000 Hz, at least about 200,000 Hz, at
least about 300,000 Hz, at least about 500,000 Hz, at least about 750,000 Hz, at least
about 1,000,000 Hz, at least about 1,500,000 Hz, at least about 2,000,000 Hz, or at
least about 3,000,000 Hz.
[0046] In some cases, the acoustic waves may be surface acoustic waves. The surface acoustic
waves may be created using a surface acoustic wave generator such as an interdigitated
transducer, and/or a material such as a piezoelectric substrate. In one set of embodiments,
the piezoelectric substrate may be isolated from the substrate except at or proximate
the location where the acoustic waves are to be applied, e.g., proximate a first or
second channel, proximate a junction of two or more channels, etc. At such locations,
the substrate may be coupled to the piezoelectric substrate (or other material) by
one or more coupling regions.
[0047] Any suitable technique may be used to create a surface acoustic wave. For example,
the surface acoustic waves may be created by a generator attached to the surface of
a material. In certain embodiments, the surface acoustic wave is created by using
an interdigitated electrode or transducer able to convert electrical signals into
acoustic waves able to travel along the surface of a material, and in some cases,
the frequency of the surface acoustic waves may be controlled by controlling the spacing
of the finger repeat distance of the interdigitated electrode or transducer. The surface
acoustic waves can be formed on a piezoelectric substrate or other material that may
be coupled to a microfluidic substrate at specific locations, e.g., at locations within
the microfluidic substrate where sorting is to take place. Suitable voltages (e.g.,
sinusoidal or other periodically varying voltages) are applied to the piezoelectric
substrate, which converts the electrical signals into mechanical vibrations, i.e.,
surface acoustic waves or sound. The sound is then coupled to the microfluidic substrate,
e.g., from the surface of the material. In the microfluidic substrate, the vibrations
pass into liquid within microfluidic channels in the microfluidic substrate (e.g.,
liquid containing cells or other species to be sorted), which give rise to internal
streaming or scattering within the fluid. In some cases, the amount of scattering
may be greater than streaming. Thus, by controlling the applied voltage, streaming
and/or scattering within the microfluidic channel may be controlled, which may be
used in some embodiments to direct or sort species within the microfluidic channel.
[0048] An interdigitated transducer typically comprises one, two, or more electrodes containing
a plurality of "fingers" extending away from the electrode, wherein at least some
of the fingers are interdigitated. The fingers may be of any length, and may independently
have the same or different lengths. The fingers may be spaced on the transducer regularly
or irregularly. In some cases, the fingers may be substantially parallel, although
in other embodiments they need not be substantially parallel. For example, in one
set of embodiments, the interdigitated transducer is a tapered interdigitated transducer.
In some cases, the fingers in a tapered interdigitated transducer may be arranged
such that the fingers are angled inwardly, e.g., as shown in Fig. 7. Examples of such
transducers may be found, e.g., in International Patent Application No.
PCT/US2011/048804, filed August 23, 2011, entitled "Acoustic Waves in Microfluidics,"
by Weitz, et al., published as
WO 2012/027366 on March 1, 2012; and
U.S. Provisional Patent Application Serial No. 61/665,087, filed June 27, 2012, entitled
"Control of Entities Such as Droplets and Cells Using Acoustic Waves," by Weitz, et
al.
[0049] The interdigitated electrode typically includes of two interlocking comb-shaped metallic
electrodes that do not touch, but are interdigitated. The electrodes may be formed
from any suitable electrode material, for example, metals such as gold, silver, copper,
nickel, or the like. The operating frequency of the interdigitated electrode may be
determined, in some embodiments, by the ratio of the sound velocity in the substrate
to twice the finger spacing. For instance, in one set of embodiments, the finger repeat
distance may be between about 10 micrometers and about 40 micrometers, between about
10 micrometers and about 30 micrometers, between about 20 micrometers and about 40
micrometers, between about 20 micrometers and about 30 micrometers, or between about
23 micrometers and about 28 micrometers.
[0050] The interdigitated electrode may be positioned on a piezoelectric substrate, or other
material able to transmit surface acoustic waves, e.g., to a coupling region. The
piezoelectric substrate may be formed out of any suitable piezoelectric material,
for example, quartz, lithium niobate, lithium tantalate, lanthanum gallium silicate,
etc. In one set of embodiments, the piezoelectric substrate is anisotropic, and in
some embodiments, the piezoelectric substrate is a Y-cut LiNbO
3 material.
[0051] The piezoelectric substrate may be activated by any suitable electronic input signal
or voltage to the piezoelectric substrate (or portion thereof). For example, the input
signal may be one in which a periodically varying signal is used, e.g., to create
corresponding acoustic waves. For instance, the signals may be sine waves, square
waves, sawtooth waves, triangular waves, or the like. The frequency may be for example,
between about 50 Hz and about 100 KHz, between about 100 Hz and about 2 kHz, between
about 100 Hz and about 1,000 Hz, between about 1,000 Hz and about 10,000 Hz, between
about 10,000 Hz and about 100,000 Hz, or the like, and/or combinations thereof. In
some cases, the frequency may be at least about 50 Hz, at least about 100 Hz, at least
about 300 Hz, at least about 1,000 Hz, at least about 3,000 Hz, at least about 10,000
Hz, at least about 30,000 Hz, at least about 100,000 Hz, at least about 300,000 Hz,
at least about 1 MHz, at least about 3 MHz, at least about 10 MHz, at least about
30 MHz, at least about 100 MHz, at least about 300 MHz, or at least about 1 GHz or
more in some embodiments. In certain instances, the frequency may be no more than
about 1 GHz, no more than about 300 MHz, no more than about 100 MHz, no more than
about 30 MHz, no more than about 10 MHz, no more than about 3 MHz, no more than about
1 MHz, no more than about 300,000 Hz, no more than about 100,000 Hz, no more than
about 30,000 Hz, no more than about 10,000 Hz, no more than about 3,000 Hz, no more
than about 1,000 Hz, no more than about 300 Hz, no more than about 100 Hz, or the
like.
[0052] The interdigitated electrode may be positioned on the piezoelectric substrate (or
other suitable material) such that acoustic waves produced by the interdigitated electrodes
are directed at a region of acoustic coupling between the piezoelectric substrate
and the microfluidic substrate. For example, the piezoelectric substrate and the microfluidic
substrate may be coupled or physically bonded to each other, for example, using ozone
plasma treatment, or other suitable techniques. In some cases, the rest of the piezoelectric
substrate and the microfluidic substrate are at least acoustically isolated from each
other, and in certain embodiments, the piezoelectric substrate and the microfluidic
substrate are physically isolated from each other. Without wishing to be bound by
any theory, it is believed that due to the isolation, acoustic waves created by the
interdigitated electrode and the piezoelectric substrate do not affect the microfluidic
substrate except at regions where it is desired that the acoustic waves are applied,
e.g., at a channel or a junction.
[0053] The coupling region, if one is present, may have any suitable shape and/or size.
The coupling region may be round, oval, or have other shapes, depending on the embodiment.
In some cases, two, three, or more coupling regions may be used. In one set of embodiments,
the coupling region is sized to be contained within a microfluidic channel. In other
embodiments, however, the coupling region may be larger. The coupling region may be
positioned within a channel or proximate to the channel, in some embodiments. See,
e.g., Int. Pat. Apl. Ser. No.
PCT/US2011/048804, filed August 23, 2011, entitled "Acoustic Waves in Microfluidics,"
by Weitz, et al., published as
WO 2012/027366 on March 1, 2012.
[0054] In some cases, control of the species may be achieved by using a tapered interdigitated
transducer. A tapered interdigitated transducer may allow relatively high control
of the location at which a SAW is applied to a channel, in contrast to an interdigitated
transducer where all of the fingers are parallel to each other and the spacing between
electrodes is constant. Without wishing to be bound by any theory, it is believed
that the location which a SAW can be applied by an interdigitated transducer is controlled,
at least in part, by the spacing between the electrodes. By controlling the potential
applied to the interdigitated transducer, and thereby controlling the resonance frequency
of the applied SAW, the position and/or the strength of the SAW as applied by the
interdigitated transducer may be correspondingly controlled. Thus, for example, applying
a first voltage to an interdigitated transducer may cause a first resonance frequency
of the resulting SAW to be applied (e.g., within a channel), while applying a second
voltage may cause a second resonance frequency of the resulting SAW to be applied
to a different location (e.g., within the channel). As another example, a plurality
of coupling regions may be used, e.g., in combination with one or more tapered interdigitated
transducers.
[0055] The microfluidic substrate may be any suitable substrate which contains or defines
one or more microfluidic channels. For instance, as is discussed below, the microfluidic
substrate may be formed out of polydimethylsiloxane, polytetrafluoroethylene, or other
suitable elastomeric polymers, at least according to various non-limiting examples.
[0056] In some embodiments, a species may be determined or sensed in some fashion, and based
on that determination, the species sorted or directed to a first location (e.g., a
first outlet) or a second location (e.g., a second outlet), e.g., using acoustic waves
The species may be determined, for example using one or more sensors that can sense
and/or determine one or more characteristics of the species, and/or a characteristic
of a portion of the fluidic system containing the species (e.g., the liquid surrounding
the species) in such a manner as to allow the determination of one or more characteristics
of the species. Characteristics determinable with respect to the species can be identified
by those of ordinary skill in the art. Non-limiting examples of such characteristics
include fluorescence, spectroscopy (e.g., optical, infrared, ultraviolet, etc.), radioactivity,
mass, volume, density, temperature, viscosity, pH, concentration of a substance, such
as a biological substance (for instance, a protein, a nucleic acid, etc.), or the
like. In some cases, the sensor may be connected to a processor, which in turn, cause
acoustic waves to be applied (or not applied).
[0057] One or more sensors and/or processors may be positioned to be in sensing communication
with species suspected of being present within a channel. "Sensing communication,"
as used herein, means that the sensor may be positioned anywhere such that the species
within the fluidic system (for example, within a channel), and/or a portion of the
fluid containing the species may be sensed and/or determined in some fashion. For
example, the sensor may be in sensing communication with the species and/or the portion
of the fluid containing the species fluidly, optically or visually, thermally, pneumatically,
electronically, or the like. The sensor can be positioned proximate a fluid containing
the species, for example, embedded within or integrally connected to a wall of a channel,
or positioned separately from the fluid but with physical, electrical, and/or optical
communication with the fluid so as to be able to sense and/or determine the species
and/or a portion of the fluid containing the species. For example, a sensor may be
free of any physical connection with a channel containing a species, but may be positioned
so as to detect electromagnetic radiation arising from the species or the fluid, such
as infrared, ultraviolet, or visible light. The electromagnetic radiation may be produced
by the species, and/or may arise from other portions of the fluid (or externally of
the fluid) and interact with the species and/or the portion of the fluid containing
the species in such as a manner as to indicate one or more characteristics of the
species, for example, through absorption, reflection, diffraction, refraction, fluorescence,
phosphorescence, changes in polarity, phase changes, changes with respect to time,
etc. As an example, a laser may be directed towards the species and/or a fluid surrounding
the species, and the fluorescence of the species and/or the surrounding fluid may
be determined. "Sensing communication," as used herein may also be direct or indirect.
As an example, light from a species may be directed to a sensor, or directed first
through a fiber optic system, a waveguide, etc., before being directed to a sensor.
[0058] Non-limiting examples of sensors useful in the invention include optical or electromagnetically-based
systems. For example, the sensor may be a fluorescence sensor (e.g., stimulated by
a laser), a microscopy system (which may include a camera or other recording device),
or the like. As another example, the sensor may be an electronic sensor, for instance,
a sensor able to determine an electric field or other electrical characteristic. For
example, the sensor may detect capacitance, inductance, etc., of a species and/or
the portion of the fluidic system containing the species.
[0059] As used herein, a "processor" or a "microprocessor" is any component or device able
to receive a signal from one or more sensors, store the signal, and/or direct one
or more responses (e.g., as described above), for example, by using a mathematical
formula or an electronic or computational circuit. The signal may be any suitable
signal indicative of the environmental factor determined by the sensor, for example
a pneumatic signal, an electronic signal, an optical signal, a mechanical signal,
etc.
[0060] A variety of definitions are now provided which will aid in understanding various
aspects of the invention. Following, and interspersed with these definitions, is further
disclosure that will more fully describe the invention.
[0061] As used herein, the term "fluid" generally refers to a substance that tends to flow
and to conform to the outline of its container, i.e., a liquid, a gas, a viscoelastic
fluid, etc. Typically, fluids are materials that are unable to withstand a static
shear stress, and when a shear stress is applied, the fluid experiences a continuing
and permanent distortion. The fluid may have any suitable viscosity that permits flow.
If two or more fluids are present, each fluid may be independently selected among
essentially any fluids (liquids, gases, and the like) by those of ordinary skill in
the art, by considering the relationship between the fluids. The fluids may each be
miscible or immiscible. For example, two fluids can be selected to be essentially
immiscible within the time frame of formation of a stream of fluids, or within the
time frame of reaction or interaction. Where the portions remain liquid for a significant
period of time, then the fluids should be essentially immiscible. Where, after contact
and/or formation, the dispersed portions are quickly hardened by polymerization or
the like, the fluids need not be as immiscible. Those of ordinary skill in the art
can select suitable miscible or immiscible fluids, using contact angle measurements
or the like, to carry out the techniques of the invention.
[0062] As used herein, a first entity is "surrounded" by a second entity if a closed planar
loop can be drawn around the first entity through only the second entity. A first
entity is "completely surrounded" if closed loops going through only the second entity
can be drawn around the first entity regardless of direction (orientation of the loop).
In one embodiment, the first entity is a cell, for example, a cell suspended in media
is surrounded by the media. In another embodiment, the first entity is a particle.
In yet another embodiment, the first entity is a fluid. The second entity may also
be a fluid in some cases (e.g., as in a suspension, an emulsion, etc.), for example,
a hydrophilic liquid may be suspended in a hydrophobic liquid, a hydrophobic liquid
may be suspended in a hydrophilic liquid, a gas bubble may be suspended in a liquid,
etc. Typically, a hydrophobic liquid and a hydrophilic liquid are essentially immiscible
with respect to each other, where the hydrophilic liquid has a greater affinity to
water than does the hydrophobic liquid. Examples of hydrophilic liquids include, but
are not limited to, water and other aqueous solutions comprising water, such as cell
or biological media, salt solutions, etc., as well as other hydrophilic liquids such
as ethanol. Examples of hydrophobic liquids include, but are not limited to, oils
such as hydrocarbons, silicone oils, mineral oils, fluorocarbon oils, organic solvents
etc. Other examples of suitable fluids have been previously described.
[0063] Similarly, a "droplet," as used herein, is an isolated portion of a first fluid that
is completely surrounded by a second fluid. It is to be noted that a droplet is not
necessarily spherical, but may assume other shapes as well, for example, depending
on the external environment. In one embodiment, the droplet has a minimum cross-sectional
dimension that is substantially equal to the largest dimension of the channel perpendicular
to fluid flow in which the droplet is located.
[0064] As mentioned, in some, but not all embodiments, the systems and methods described
herein may include one or more microfluidic components, for example, one or more microfluidic
channels. "Microfluidic," as used herein, refers to a device, apparatus or system
including at least one fluid channel having a cross-sectional dimension of less than
1 mm, and a ratio of length to largest cross-sectional dimension of at least 3:1.
A "microfluidic channel," as used herein, is a channel meeting these criteria. The
"cross-sectional dimension" of the channel is measured perpendicular to the direction
of fluid flow within the channel. Thus, some or all of the fluid channels in microfluidic
embodiments of the invention may have maximum cross-sectional dimensions less than
2 mm, and in certain cases, less than 1 mm. In one set of embodiments, all fluid channels
containing embodiments of the invention are microfluidic or have a largest cross sectional
dimension of no more than 2 mm or 1 mm. In certain embodiments, the fluid channels
may be formed in part by a single component (e.g. an etched substrate or molded unit).
Of course, larger channels, tubes, chambers, reservoirs, etc. can be used to store
fluids and/or deliver fluids to various components or systems of the invention. In
one set of embodiments, the maximum cross-sectional dimension of the channel(s) containing
embodiments of the invention is less than 500 microns, less than 200 microns, less
than 100 microns, less than 50 microns, or less than 25 microns.
[0065] A "channel," as used herein, means a feature on or in an article (substrate) that
at least partially directs flow of a fluid. The channel can have any cross-sectional
shape (circular, oval, triangular, irregular, square or rectangular, or the like)
and can be covered or uncovered. In embodiments where it is completely covered, at
least one portion of the channel can have a cross-section that is completely enclosed,
or the entire channel may be completely enclosed along its entire length with the
exception of its inlet(s) and/or outlet(s). A channel may also have an aspect ratio
(length to average cross sectional dimension) of at least 2:1, more typically at least
3:1, 5:1, 10:1, 15:1, 20:1, or more. An open channel generally will include characteristics
that facilitate control over fluid transport, e.g., structural characteristics (an
elongated indentation) and/or physical or chemical characteristics (hydrophobicity
vs. hydrophilicity) or other characteristics that can exert a force (e.g., a containing
force) on a fluid. The fluid within the channel may partially or completely fill the
channel. In some cases where an open channel is used, the fluid may be held within
the channel, for example, using surface tension (i.e., a concave or convex meniscus).
[0066] The channel may be of any size, for example, having a largest dimension perpendicular
to fluid flow of less than about 5 mm or 2 mm, or less than about 1 mm, or less than
about 500 microns, less than about 200 microns, less than about 100 microns, less
than about 60 microns, less than about 50 microns, less than about 40 microns, less
than about 30 microns, less than about 25 microns, less than about 10 microns, less
than about 3 microns, less than about 1 micron, less than about 300 nm, less than
about 100 nm, less than about 30 nm, or less than about 10 nm. In some cases the dimensions
of the channel may be chosen such that fluid is able to freely flow through the article
or substrate. The dimensions of the channel may also be chosen, for example, to allow
a certain volumetric or linear flowrate of fluid in the channel. Of course, the number
of channels and the shape of the channels can be varied by any method known to those
of ordinary skill in the art. In some cases, more than one channel or capillary may
be used. For example, two or more channels may be used, where they are positioned
inside each other, positioned adjacent to each other, positioned to intersect with
each other, etc.
[0067] In one set of embodiments, the species are cells or other entities, such as proteins,
viruses, macromolecules, particles, etc. As used herein, a "cell" is given its ordinary
meaning as used in biology. The cell may be any cell or cell type. For example, the
cell may be a bacterium or other single-cell organism, a plant cell, or an animal
cell. If the cell is a single-cell organism, then the cell may be, for example, a
protozoan, a trypanosome, an amoeba, a yeast cell, algae, etc. If the cell is an animal
cell, the cell may be, for example, an invertebrate cell (e.g., a cell from a fruit
fly), a fish cell (e.g., a zebrafish cell), an amphibian cell (e.g., a frog cell),
a reptile cell, a bird cell, or a mammalian cell such as a primate cell, a bovine
cell, a horse cell, a porcine cell, a goat cell, a dog cell, a cat cell, or a cell
from a rodent such as a rat or a mouse. If the cell is from a multicellular organism,
the cell may be from any part of the organism. For instance, if the cell is from an
animal, the cell may be a cardiac cell, a fibroblast, a keratinocyte, a heptaocyte,
a chondracyte, a neural cell, a osteocyte, a muscle cell, a blood cell, an endothelial
cell, an immune cell (e.g., a T-cell, a B-cell, a macrophage, a neutrophil, a basophil,
a mast cell, an eosinophil), a stem cell, etc. In some cases, the cell may be a genetically
engineered cell. In certain embodiments, the cell may be a Chinese hamster ovarian
("CHO") cell or a 3T3 cell.
[0068] A variety of materials and methods, according to certain aspects of the invention,
can be used to form any of the above-described components of the systems and devices
of the invention. In some cases, the various materials selected lend themselves to
various methods. For example, various components of the invention can be formed from
solid materials, in which the channels can be formed via micromachining, film deposition
processes such as spin coating and chemical vapor deposition, laser fabrication, photolithographic
techniques, etching methods including wet chemical or plasma processes, and the like.
See, for example,
Scientific American, 248:44-55, 1983 (Angell, et al). In one embodiment, at least a portion of the fluidic system is formed of
silicon by etching features in a silicon chip. Technologies for precise and efficient
fabrication of various fluidic systems and devices of the invention from silicon are
known. In another embodiment, various components of the systems and devices of the
invention can be formed of a polymer, for example, an elastomeric polymer such as
polydimethylsiloxane ("PDMS"), polytetrafluoroethylene ("PTFE" or Teflon
®), or the like.
[0069] Different components can be fabricated of different materials. For example, a base
portion including a bottom wall and side walls can be fabricated from an opaque material
such as silicon or PDMS, and a top portion can be fabricated from a transparent or
at least partially transparent material, such as glass or a transparent polymer, for
observation and/or control of the fluidic process. Components can be coated so as
to expose a desired chemical functionality to fluids that contact interior channel
walls, where the base supporting material does not have a precise, desired functionality.
For example, components can be fabricated as illustrated, with interior channel walls
coated with another material. Material used to fabricate various components of the
systems and devices of the invention, e.g., materials used to coat interior walls
of fluid channels, may desirably be selected from among those materials that will
not adversely affect or be affected by fluid flowing through the fluidic system, e.g.,
material(s) that is chemically inert in the presence of fluids to be used within the
device.
[0070] In one embodiment, various components of the invention are fabricated from polymeric
and/or flexible and/or elastomeric materials, and can be conveniently formed of a
hardenable fluid, facilitating fabrication via molding (e.g. replica molding, injection
molding, cast molding, etc.). The hardenable fluid can be essentially any fluid that
can be induced to solidify, or that spontaneously solidifies, into a solid capable
of containing and/or transporting fluids contemplated for use in and with the fluidic
network. In one embodiment, the hardenable fluid comprises a polymeric liquid or a
liquid polymeric precursor (i.e. a "prepolymer"). Suitable polymeric liquids can include,
for example, thermoplastic polymers, thermoset polymers, or mixture of such polymers
heated above their melting point. As another example, a suitable polymeric liquid
may include a solution of one or more polymers in a suitable solvent, which solution
forms a solid polymeric material upon removal of the solvent, for example, by evaporation.
Such polymeric materials, which can be solidified from, for example, a melt state
or by solvent evaporation, are well known to those of ordinary skill in the art. A
variety of polymeric materials, many of which are elastomeric, are suitable, and are
also suitable for forming molds or mold masters, for embodiments where one or both
of the mold masters is composed of an elastomeric material. A non-limiting list of
examples of such polymers includes polymers of the general classes of silicone polymers,
epoxy polymers, and acrylate polymers. Epoxy polymers are characterized by the presence
of a three-membered cyclic ether group commonly referred to as an epoxy group, 1,2-epoxide,
or oxirane. For example, diglycidyl ethers of bisphenol A can be used, in addition
to compounds based on aromatic amine, triazine, and cycloaliphatic backbones. Another
example includes the well-known Novolac polymers. Non-limiting examples of silicone
elastomers suitable for use according to the invention include those formed from precursors
including the chlorosilanes such as methylchlorosilanes, ethylchlorosilanes, phenylchlorosilanes,
etc.
[0071] Silicone polymers are preferred in one set of embodiments, for example, the silicone
elastomer polydimethylsiloxane. Non-limiting examples of PDMS polymers include those
sold under the trademark Sylgard by Dow Chemical Co., Midland, MI, and particularly
Sylgard 182, Sylgard 184, and Sylgard 186. Silicone polymers including PDMS have several
beneficial properties simplifying fabrication of the microfluidic structures of the
invention. For instance, such materials are inexpensive, readily available, and can
be solidified from a prepolymeric liquid via curing with heat. For example, PDMSs
are typically curable by exposure of the prepolymeric liquid to temperatures of about,
for example, about 65 °C to about 75 °C for exposure times of, for example, about
an hour. Also, silicone polymers, such as PDMS, can be elastomeric and thus may be
useful for forming very small features with relatively high aspect ratios, necessary
in certain embodiments of the invention. Flexible (e.g., elastomeric) molds or masters
can be advantageous in this regard.
[0072] One advantage of forming structures such as microfluidic structures of the invention
from silicone polymers, such as PDMS, is the ability of such polymers to be oxidized,
for example by exposure to an oxygen-containing plasma such as an air plasma, so that
the oxidized structures contain, at their surface, chemical groups capable of cross-linking
to other oxidized silicone polymer surfaces or to the oxidized surfaces of a variety
of other polymeric and non-polymeric materials. Thus, components can be fabricated
and then oxidized and essentially irreversibly sealed to other silicone polymer surfaces,
or to the surfaces of other substrates reactive with the oxidized silicone polymer
surfaces, without the need for separate adhesives or other sealing means. In most
cases, sealing can be completed simply by contacting an oxidized silicone surface
to another surface without the need to apply auxiliary pressure to form the seal.
That is, the pre-oxidized silicone surface acts as a contact adhesive against suitable
mating surfaces. Specifically, in addition to being irreversibly sealable to itself,
oxidized silicone such as oxidized PDMS can also be sealed irreversibly to a range
of oxidized materials other than itself including, for example, glass, lithium niobate,
silicon, silicon oxide, quartz, silicon nitride, polyethylene, polystyrene, glassy
carbon, and epoxy polymers, which have been oxidized in a similar fashion to the PDMS
surface (for example, via exposure to an oxygen-containing plasma). Oxidation and
sealing methods useful in the context of the present invention, as well as overall
molding techniques, are described in the art.
[0073] Another advantage to forming microfluidic structures of the invention (or interior,
fluid-contacting surfaces) from oxidized silicone polymers is that these surfaces
can be much more hydrophilic than the surfaces of typical elastomeric polymers (where
a hydrophilic interior surface is desired). Such hydrophilic channel surfaces can
thus be more easily filled and wetted with aqueous solutions than can structures comprised
of typical, unoxidized elastomeric polymers or other hydrophobic materials.
[0074] In one embodiment, a bottom wall is formed of a material different from one or more
side walls or a top wall, or other components. For example, the interior surface of
a bottom wall can comprise the surface of a silicon wafer or microchip, or other substrate.
Other components can, as described above, be sealed to such alternative substrates.
Where it is desired to seal a component comprising a silicone polymer (e.g. PDMS)
to a substrate (bottom wall) of different material, the substrate may be selected
from the group of materials to which oxidized silicone polymer is able to irreversibly
seal (e.g., glass, silicon, silicon oxide, quartz, silicon nitride, polyethylene,
polystyrene, epoxy polymers, and glassy carbon surfaces which have been oxidized).
Alternatively, other sealing techniques can be used, as would be apparent to those
of ordinary skill in the art, including, but not limited to, the use of separate adhesives,
thermal bonding, solvent bonding, ultrasonic welding, etc.
[0075] The following examples are intended to illustrate certain embodiments of the present
invention, but do not exemplify the full scope of the invention.
EXAMPLE 1
[0076] By utilizing a vertical flow-focusing junction and a slanted ceiling groove, this
example illustrates enhancement of surface acoustic wave cell sorting. These devices
may be able to attain levels of performance approaching that of state of the art fluorescence-activated
cell sorters in terms of event rate and purity. This example demonstrates a microfluidic
cell sorter, which screens cells at rates approaching those of commercially-available
FACS. This device incorporates a three-dimensional flow-focusing nozzle with a slanted
ceiling groove to enhance the capabilities of a SAW transducer by harnessing the component
of the SAW oriented normal to the plane of the substrate. This example determines
the conditions for device performance, and uses these principles to implement a cell
sorter. The device achieves sorting at a rate of 9000 events/s with 55% purity and
yields 90% purity, while operating at 1000 events/s.
[0077] Without wishing to be bound by any theory, it is believed that when a SAW impinges
on the flow of liquid within a microfluidic device, it refracts, forming a longitudinal
acoustic wave in the liquid. It is this acoustic wave that can deflect cells. The
angle of refraction for SAW is known as the Rayleigh angle, θ
R, and it depends on the speed of sound in the liquid,
vl, and the speed of the SAW,
vs, according to Snell's law,
sin θR =
v1/
vs. In the materials used for SAW microfluidics, the SAW travels along the substrate
surface faster than the acoustic wave propagates in the liquid, so the Rayleigh angle
is small and the refracted wave is directed closer to the substrate's surface normal
than to the plane of the substrate. As a result, the normal component of the refracted
acoustic wave is larger than the parallel component in general. The substrate plane
is also constrains the design of the flow channel, because microfluidic channels made
by lithographic techniques are defined by masks that are usually two dimensional.
Moreover, microfluidic devices are assembled such that the lithographic plane is parallel
to the substrate plane. Therefore, most microfluidic devices utilize the component
of the acoustic wave parallel to the substrate for particle manipulations.
[0078] To exploit the component of the acoustic wave normal to the substrate, this example
uses multi-layer microfluidic devices. A multi-layer SAW device, which exploits the
normal component of SAW for sorting, can obtain enhanced sorting performance compared
to existing designs, because it channels more of the available power into actuating
cells.
[0079] This example implements a multi-layer device geometry that utilizes the normal component
of the acoustic wave for cell sorting applications, illustrated in Fig. 1. Here, a
tapered interdigital transducer (IDT) can generate surface acoustic waves that can
actuate particles, cells, or other species. (Cells are used here and in the following
examples by way of example only, and are intended to be illustrative and not limiting.)
In the tapered IDT design, a range of frequencies can excite SAWs, at different positions
along the transducer, because the resonant wavelength, defined by the pitch of the
electrodes, varies along the transducer. The slope at which the IDT tapers determines
the aperture of the SAW, by limiting the area of the transducer in which a given frequency
resonates. The IDT is positioned directly adjacent to the microfluidic device's sorting
channel to increase the amount of power that gets transferred to the liquid, by minimizing
the distance the SAW must travel before it refracts into the liquid in the channel,
as shown in Fig. 1A. The fingers of the IDT are situated beneath an air gap, to prevent
the power carried by the SAW from leaking into the device prematurely. The flow channel
of the microfluidic device contains micro-fabricated features, which enable the device
to utilize the normal component of the acoustic wave, a slanted ceiling groove and
a vertical flow-focusing nozzle. Their positions with respect to the IDT and the sorting
channel as well as the air gap are shown in Fig. 1B.
[0080] The slanted groove generates a flow with a velocity profile that varies strongly
with height; within the ceiling groove, fluid flows along the length of the groove,
while the flow at the bottom of the sorting channel remains largely unperturbed. Consequently,
it is the slanted groove, which harnesses the normal component of the acoustic wave,
because the acoustic wave pushes cells to the top of the channel, where they interact
with the flow within the groove. Thus, the groove ensures that the height at which
a cell passes through the sorting channel determines whether it is discarded or retained.
The slanted groove is presented in more detail in Fig. 1C. The slanted groove must
be paired with a vertical flow-focusing nozzle, to ensure that only target cells interact
with the groove. The cell inlet channel of the vertical flow focusing nozzle is fabricated
at a lower height than the channels carrying sheath fluid. When the sheath channels
intersect the cell inlet, at the entrance to the sorting channel, the sheath fluid
focuses the cell flow laterally and vertically into a narrow thread at the bottom
of the sorting channel. The sheath channels form a Y-shape with the sorting channel,
which eliminates stagnation points just after the nozzle. The nozzle is offset from
the midline of the channel, so that variations in flow rate or other unexpected perturbations
will not cause cells to enter the retention channel spuriously. The nozzle geometry
is depicted in Fig. 1D.
[0081] In the absence of surface acoustic waves, a cell passing through the device does
not interact with the ceiling groove; it transits directly through the sorting channel
and out of the device via the waste outlet unperturbed. When a cell of interest is
detected, a pulse of SAW is applied, and the normal component of the resulting acoustic
wave pushes the particle to the top of the sorting channel, where advection carries
it across the sorting channel; this cell then exits the device through the retention
outlet, where it can be recovered. In contrast with previous slanted groove microfluidic
devices, which use arrays of slanted grooves to direct flows or particles, here, the
interaction of cell with the groove depends on the application of the SAW pulse; the
cell is deflected completely into the groove, and a single groove is sufficient to
achieve the desired effect (although more than one groove could also be used). The
angle of the slanted groove creates a flow, which ensures that cells continuously
flow out of the device as they are sorted, unlike trapping designs, in which the desired
particles are pinned behind a vertical barrier. As a result, this offers a device
geometry uniquely adapted for rapid sorting of cells.
[0082] Fig. 1 shows a schematic of the groove-enhanced cell sorting design used in this
particular example, Here, the relative positions of the flow channels and interdigital
transducer (left/center bars) are illustrated (Fig. 1A). Metal pads (far left) connect
to the fingers of the IDT through bus bars. The flow channel has a cell inlet (upper
middle) and two sheath inlets (upper left and upper right) as well as a waste outlet
(lower right) and a retention outlet (lower right). A zoomed in view shows the positions
of the flow-focusing nozzle (left), the sorting channel (center), and the slanted
groove (above the sorting channel), and the tapered IDT fingers (bottom). The flow-focusing
nozzle is located where the two sheath flows and the cell inlet meet. The channel
bifurcates after the slanted groove. The upper channel leads to the retention outlet,
while the lower outlet leads to the waste outlet (Fig. 1B). Further details of the
slanted groove and the nozzle design are provided in Fig. 1C and 1D respectively.
EXAMPLE 2
[0083] In this example, the capabilities of the slanted groove device were tested for cell
sorting applications, by determining the conditions for which an applied SAW pulse
generally succeeds at redirecting a target cell into the retention outlet. As a basis
for testing, a device made from poly(dimethylsiloxane) (PDMS) was used, with a vertical
flow-focusing nozzle that is 50 micrometers wide and 25 micrometers tall; a sorting
channel that is 250 micrometers wide and 50 micrometers tall; and a rectangular groove
which is 120 micrometers wide, rises 25 micrometers above the sorting channel (e.g.,
which can contain a cell), and is tilted 60° from the overall direction of flow. These
dimensions are not intended to be limiting. The instrument triggers a SAW pulse whenever
it detects a cell of interest, e.g., due to fluorescence, and the trajectories of
individual cells are captured using a high-speed camera. Each resulting movie was
analyzed to extract the trajectory of the target cell; a given sorting event was deemed
a success if the desired cell exited the sorting channel through the retention outlet,
or a failure if the desired cell exited the sorting channel through the waste outlet.
[0084] Cell tracks showing a non-fluorescent cell proceeding through the sorting channel
to the waste outlet and a target cell being successfully pushed into the groove and
subsequently traveling along the length of the groove to the retention outlet are
shown in Fig. 2. For each of the parameters tested, the threshold value for which
the device performance becomes consistent is defined as the lowest value for which
at least 90% of the measured events are successful. The threshold value for each sorting
condition is determined on three independent days of experiment using at least 48
individual events. These experiments assess the robustness and reproducibility of
the technique under different conditions.
[0085] Fig. 2 illustrates that the slanted groove enhances surface acoustic wave (SAW) actuation.
Two single cell tracks are captured from a device with a slanted groove that rises
25 micrometers above the sorting channel. In one case, no sorting pulse is applied
(Fig. 2A), while in the other a pulse is applied (Fig. 2B. If no SAW is applied, the
cell follows the same trajectory as the bulk of the cell phase fluid. The cell passes
through the sorting channel and underneath slanted groove without deflection and exits
the device through the waste channel (lower right). When the SAW pulse is applied,
the cell is deflected into the slanted groove, where it is carried across the sorting
channel by the flow of sheath fluid within the groove. The sorted cells moves laterally
more than 150 micrometers and exits the device through the retention outlet (upper
right). The cell phase fluid is visible, because of the index of refraction difference
between the phosphate-buffered saline sheath phase and the cell phase that contains
Optiprep. The cell tracks depicted here are projections of approximately 20 frames
taken with a high speed camera at 11,267 fps. The scale bar represents 50 micrometers.
EXAMPLE 3
[0086] This example determines the minimum length of the SAW pulse required for the slanted
groove device to reproducibly actuate cells into the sorting channel for a range of
different RF power levels and cell types. As the radio frequency (RF) power used to
generate the SAW is increased, shorter pulses provide enough energy to redirect cells
into the groove. Cells can be efficiently actuated with pulses as short as 20 microseconds.
For model adherent and non-adherent cell types, cells are reproducibly deflected into
the groove with similar SAW pulse parameters, as shown in Fig. 3A. However, one cell
line consistently requires less energy for deflection than the other, which suggests
that the two cell lines may have inherent differences in their average size or acoustic
contrast. Nevertheless, the slanted groove device can actuate both adherent and non-adherent
cells and the range of parameters, for which actuation is efficient, is compatible
with high-speed sorting applications.
[0087] In this example, the total flow rate was varied to determine the effect of average
flow speed on the sorting process. For each flow rate, the length of the SAW pulse
was constant at 50 microseconds and the ratio of cell phase to sheath flow was also
held constant. The applied power was varied and the minimum power for which cells
were successfully actuated consistently was recorded.
[0088] At low flow rates, the threshold power and flow rate were essentially uncorrelated,
but at higher flow rates, there was a correlation between flow rate and applied power,
as the cell's deflection became limited by the duration of exposure to the acoustic
wave pulse. The relationship between the threshold power of the SAW pulse and the
overall device flow rate is depicted in Fig. 3B. These results show that the sorting
effect is robust at a broad range cell velocities.
[0089] The impact of groove geometry on cell actuation in this design was quantified by
varying the groove's width, height, and angle independently. Only one dimension of
the groove was changed in each set of experiments and the threshold power required
for sorting was measured, while the flow rate and the length of the sorting pulse
as well as the other groove dimensions were all kept fixed. As the groove is widened,
less power was necessary to cause the cell to interact with the flow within the groove,
as demonstrated in Fig. 3C. While it is possible to sort cells using the vertical
flow-focusing nozzle without any groove or with a very shallow groove, good sorting
results were attained with grooves fabricated at a height of 25 micrometers, shown
in Fig. 3D. Different groove angles showed no significant effect on the threshold
power required for sorting. There may be a slight variation due to changes in the
effective aperture of the groove or because the flow speed is higher in the groove
with the lower angle, but these were within the range of measurement error, and had
very little effect on the threshold power required for sorting.
[0090] These results demonstrate that both the depth and the width of the groove, but not
the groove angle, provide geometrical tuning parameters, which can influence the interaction
of cells with the groove following SAW actuation.
[0091] Fig. 3 shows cell-sorting performance of groove-enhanced devices. Sorting devices
with slanted grooves reliably actuated cells for a wide range of operating conditions.
The symbols on each plot in Fig. 3 are centered on the mean of the three independent
threshold values, while the error bars depict the full range of threshold values.
For points without visible error bars, the marker size exceeds the extent of the error
bars. The length of the pulse necessary to deflect a given cell type increases as
the applied RF power decreases. The device actuates both adherent Madin-Darby canine
kidney (MDCK; open symbols) cells and non-adherent chronic myelogenous leukemia (K-562;
filled symbols) cells with performance levels sufficient to achieve high speed cell
sorting (Fig. 3A). As the flow rate is varied, the threshold power required for sorting
increases, except at the lower range of flow rates, where it appears that there was
a minimum amount of power necessary for sorting (Fig. 3B). The threshold power for
sorting decreased linearly as the groove is widened (Fig. 3C). The threshold power
changed non-monotonically as groove height was increased (Fig. 3D), but sorting takes
place with the lowest required power for the tallest tested grooves.
EXAMPLE 4
[0092] In this example, the groove-enhanced cell sorter was operated under realistic conditions
by sorting fluorescent cells from a mixture of cells. In each experiment, a reference
library was prepared with known cell density and fraction of fluorescent K-562 cells.
The slanted groove sorter extracts only the fluorescent cells. The device was operated
with two different sheath flow rates and two different groove widths to measure how
these parameters will affect sorter performance. The purified sample was collected
and the recovered cells are imaged using a confocal microscope to obtain an independent
measurement of cell purity. To elucidate the dependence of purity of the sorted fraction
on the event rate at which the sorter was operated, this process was repeated for
reference libraries with a range of cell densities at the same sample flow rate. The
sorter was able to achieve high purity at low event rates, but the purity decreased
as the concentration of cells increases with a trend that appears linear, as shown
in Fig. 4.
[0093] The overall trend fits to a line, which intersects the purity axis at 93% and which
has a slope of -4.3% per kilohertz. Although this device used relatively high levels
of SAW power, the viability of the sorted fraction of cells remains high, greater
than 96%. At first glance, the entire data set fits adequately to a line, but the
fit averages out any effects arising from operating the device under different flow
rate conditions or using different groove widths.
[0094] To determine whether different flow rate conditions and groove widths have a minimal
influence on the recovered sample purity, the data were binned first according to
sheath flow rate and then by groove width, and examine the distributions of the residuals
for each parameter-the difference between a given data point and the fit at that point.
There was no clear difference between the purity for devices operated with different
sheath flow rates, but the devices with a narrow 40 micrometers groove consistently
extract higher purity samples than those with an 80 micrometer groove; this contrast
is evident in the box plots shown in Fig. 4. However, it should be noted that sorting
was nonetheless achieved with the 80 micrometer groove. The observation that the narrowest
groove provides improved purity suggests that the groove acts as a spatial filter;
only cells that enter the groove are carried across the sorting channel to the sorting
outlet, and cells enter the groove if they are aligned with the groove when the acoustic
wave is applied. This increases the likelihood that only the correct cell enters the
groove. This effect offers an advantage compared to previous SAW sorting designs,
in which the sorting purity can only be increased by changing the design of the SAW
transducer or the operating flow rates.
[0095] Fig. 4 illustrates cell purity v. event rate. The purity of each recovered sample
is plotted relative to the event rate at which the sample is sorted. Filled symbols
are used for samples sorted with a 40 micrometer groove device, while empty symbols
represent samples sorted with the 80 micrometer groove. Square symbols represent data
gathered with total sheath flow rates of 45 ml/h, and circles for sheath flow rates
of 60 ml/h. All of the data sets follow the same general trend.
[0096] Fig. 5 illustrates residuals for variations in flow rate and groove width. For each
data point, a residual value was determined, which measures the distance on the purity
axis from a linear fit to the entire data set. The residual data is associated into
groups based on the device operating parameters, and distributions of the residuals
from the overall trend line are plotted as box and whisker plots for each group. The
data are grouped according to the total sheath flow rate (Fig. 5A) and the slanted
groove width (Fig. 5B). The median values, represented by the lines in the center
of the boxes, are essentially identical for the two different flow rate conditions,
while the devices with the narrower groove produce samples that are about 5% more
pure than the larger groove on average.
[0097] Thus, the slanted groove-enhanced cell sorter discussed in the above examples represents
one embodiment of microfluidic cell sorters using SAWs to sort cells rapidly to high
levels of purity. The design used in these examples featured a novel mechanism for
channeling the normal component of the acoustic wave into driving cell motion. The
sorter operated at high rates, approaching those of commercial FACS instruments, and
also could achieve high purity for recovery of enriched samples. Slanted groove SAW
devices offer several routes to enhanced performance, because improvements in the
designs of the IDT, the vertical flow-focusing nozzle, and the slanted groove itself
can all be tuned and integrated to further increase overall performance. For example,
tuning the nozzle design to reduce the spread in cell velocities could lead to increases
in the sorting purity; inertial focusing devices could be used to align cells without
the need for a multi-layer nozzle design; or fully sheath-less focusing techniques
could be employed to eliminate the need for the sheath channels altogether. Likewise,
the IDT design could be improved through the use of a focusing geometry, so that the
power density is spread over a wider area, to reduce the chance that the IDT becomes
damaged during use. Like other microfluidic cell sorters, the fluid handling region
is enclosed and aerosols are not produced by the acoustic waves in the system; therefore,
the sorter could find application in screening bio-hazardous samples without the need
for additional containment measures. The current design is disposable, but to completely
eliminate the risk of cross-contamination, the IDT also needs to be discarded or sterilized.
This issue can be solved, for example, by bonding the PDMS flow channel to a PDMS
membrane with a micro-fabricated post that channels the SAW from the IDT into the
flow channel where it can deflect cells. Then the PDMS flow channel is fully disposable,
while the IDT can be retained, all while maintaining sterile operating conditions.
SAW cell sorters are also amenable to parallelization, in which multiple unit cells
work together in parallel to produce a single sorter with enhanced aggregate performance.
Each SAW unit cell requires only a few components, either a voltage-controlled oscillator,
a RF switch, and an RF amplifier. By combining tens or hundreds of unit cells, a parallelized
instrument could truly achieve unprecedented sorting rates. Moreover, the same SAW
device platform is compatible with both cells and droplets, meaning a single instrument
could provide users with both FACS and droplet sorting capabilities.
EXAMPLE 5
[0098] This example, illustrates various experimental techniques used in the above examples.
[0099] Device Design. Drawings for both IDTs and microfluidic channels are created using
AutoCAD (Autodesk, Inc., San Rafael, CA). The spacing of the fingers in the IDT design
are chosen such that the resonant frequency varies linearly along the transducer between
161 and 171 MHz. Bus bars on either side of the IDT connect to square pads with 1.5
mm side length, through which external voltages are applied to all the IDT fingers
with minimal resistance. Additional markings delimit each transducer so that the IDTs
can be cut from the wafer into individual squares with 17.4 mm side length. The design
is etched into a chrome mask (Photo-Sciences Inc., Torrance, CA) to ensure that the
actual finger widths closely match the designed values. The microfluidic device has
three layers, each fabricated using a separate lithographic mask. The first layer
contains only the nozzle, because the nozzle is shallower than the rest of the device.
The nozzle extends underneath both the cell inlet region and the sorting channel to
ensure that the nozzle is insensitive to the alignment of subsequent layers. The nozzle
is designed to be nominally 40 micrometers long reducing the chance that cells will
clog the nozzle. Most of the other features are on the device's second layer, including
the air gap for the fingers of the IDT, the sheath and cell inlets, the sorting channel,
and the device outlets. The third layer only contains the slanted groove, which is
patterned on top of the sorting channel. The groove is drawn 230 micrometers wide,
slightly less than the full sorting channel width, ensuring that even if the groove
is slightly misaligned from the sorting channel, the wall of the channel where the
acoustic wave encounters the liquid will not be distorted. Distortions of the channel
wall could refract the acoustic wave at unexpected angles. Each layer contains at
least two sets of alignment marks consisting of an asymmetrical pattern of crosses,
enabling different layers to be aligned precisely to the same position. The masks
for the individual microfluidic device layers are ordered from CAD/Art Services, Inc.
(Bandon, OR) and imaged with a resolution of 25,400 dpi.
[0100] Transducer Fabrication. Interdigital transducers are fabricated using a lift-off
process, described in the protocol from the Center for Nanoscale Systems at Harvard
University. The substrates are black lithium niobate wafers (Precision Micro-Optics,
LLC, Woburn, MA) with 4 inch diameter and 128° Y-cut. Black lithium niobate is effective
in SAW applications and exhibits less pyroelectric effect, making it easier to handle.
The wafers are cleaned on the spin coater using acetone, then isopropanol, and spun
dry. Residual moisture is removed with a dehydration bake at 180 °C for 1 minute.
The rate of temperature change was eased by placing the wafer on a hot plate at 115
°C for 1 minute just prior to and immediately following baking at 180 °C. Resist is
dispensed onto the wafer using a disposable dropper. A layer of LOR3A resist (MicroChem,
Westborough, MA) is added to the wafer surface; then, the wafer is spun at 4000 rpm
to create a layer 300 nm thick. The resist was baked at 180 °C for 4 minutes, using
the same temperature ramping method as the dehydration bake. A layer of Shipley 1805
(MicroChem, Westborough, MA) was added and spun at 4000 rpm. This layer was baked
for 1 minute at 115 °C. The photoresists were patterned using the IDT chrome mask
on a mask aligner (MJB4, Karl Suss, Garching, Germany). The pattern was developed
by immersing the wafer in CD-26 developer (Microposit, Austin, TX) for 75 s to form
a shadow mask for E-beam deposition. The wafer was rinsed clean with water and blown
dry with nitrogen. The exposed surface of the wafer was cleaned using an oxygen plasma
cleaner (SCE106, Anatech, Union City, CA) with 75 W of RF power and an oxygen gas
flow rate of 40 sccm for 20 s. 10 nm of titanium was deposited as an adhesion layer,
followed by 50 nm of gold using an E-beam evaporator (Denton Vacuum LLC, Moorestown,
NJ) to form electrodes on the wafer surface. The photoresist was then lifted off by
soaking the wafer in Remover-PG (MicroChem, Westborough, MA) at 80 °C for about 60
minutes. A layer of Shipley 1813 was added, and baked at 115 °C for 1 minute to form
a protective layer. The patterned substrates was scored using a dicing saw (Disco
DAD321, Tokyo, JPN) to make cuts 250 micrometers deep in the lithium niobate. The
wafer broke cleanly along the scored lines, yielding up to 21 devices per wafer. The
IDTs were cleaned with acetone to remove the protective layer prior to use.
[0101] Soft lithography. Multi-layer lithography was performed to create molds for PDMS
replicas. The layers were processed following the method recommended in the manufacturer's
data sheet for SU-8 3025 resist (MicroChem, Westborough, MA). For each layer, a small
amount of resist was dispensed onto the wafer. The wafer was spun at 3000 rpm to create
a layer of resist that was 25 micrometers thick. Each layer was pre-baked for a total
of 12 minutes at 95 °C, rotating the wafer on the hot plate after half the bake time
has elapsed. The layer was then aligned to any underlying features and expose new
features using a mask aligner (ABM, Scotts Valley, CA). The resist was then baked
for 1 minute at 65 °C and 5 minutes at 95 °C. At this point, additional layers could
be added on top of the previous ones. Once all layers were exposed and all baking
steps were complete, the features were developed by immersing the wafer in polyethylene
glycol monomethyl ether acetate for 5 minutes using an orbital shaker (Roto Mix 8x8,
Thermo Fisher, Waltham, MA) to agitate the developer. After developing, the wafer
was rinsed with isopropanol and blown dry with nitrogen. The wafer now served as a
mold for creating replicas in PDMS. PDMS (Sylgard 184, Dow-Corning, Midland, MI) base
and cross-linker was mixed in a 10:1 ratio using a Thinky mixer (AR-100, Thinky Corporation,
Tokyo, Japan). The mixer was run in mixing mode for 30 s and degassing mode for another
30 s. The mold was placed in a plastic petri dish and the uncured PDMS poured on top.
The PDMS was degassed for 10 minutes, then place the dish in an oven at 65 °C overnight.
Once the PDMS is cured, the edges of the wafer were cut around using a scalpel and
the PDMS replica lifted out of the mold. Each PDMS replica contained 16 independent
devices; the replica was cut into individual flow channels prior to use. Interface
holes were created with a biopsy punch (Uni-Core, GE Healthcare Life Sciences, Pittsburgh,
PA). 0.75 mm diameter holes were used for the inlets and 1.5 mm diameter holes used
for the outlets. Once the interface holes were formed, individual PDMS flow channels
could be mounted into the sample holder.
[0102] Sorting Apparatus. The microscope body of the sorting apparatus was built from modular
optical components. Fluorescence was excited by a 473 nm laser (Laserglow Technologies,
Toronto, ON) with 100 mW output. The laser beam was expanded by a beam expander (BE-05-10-A,
Thorlabs Inc., Newton, NJ), and steered into the body of the microscope. Excitation
light reflected off the excitation dichroic (FF495-Di03-25x36, Semrock, Inc., Buffalo,
NY) and up through the objective. A cylindrical achromat (ACY254-200-A, Thorlabs Inc.,
Newton, NJ) focused one axis of the beam into a line in the back aperture of a microscope
objective (Nikon 10X/0.45NA). The objective focused the excitation light into a line
in the microscope's focal plane and collected any resulting fluorescence emission
from the sample. The emitted fluorescence passed through the excitation dichroic,
but reflected off the fluorescence dichroic (FF605-Di01-25x36, Semrock, Inc., Buffalo,
NY); the fluorescence passed through a colored glass longpass filter (FGL495, Thorlabs
Inc., Newton, NJ) and a dielectric bandpass filter (FF01-520/44-25, Semrock, Inc.,
Buffalo, NY) illuminating the photocathode of a photomultiplier tube (H10723-20, Hamamatsu
Photonics K.K., Hamamatsu, Japan), while noise sources of light were attenuated by
the filters. The microscope's field of view was illuminated using an infrared light
emitting diode. The infrared light passed through both of the microscope's dichroic
filters, and reflected from a turning mirror (CM1-P01, Thorlabs Inc.). The infrared
image was focused onto the sensor of a fast camera (HiSpec1, Fastec Imaging, San Diego,
CA) by a tube lens (AC254-100-B-ML, Thorlabs Inc.) to allow videos of the sorting
process to be recorded at high speed. A Leica manual stage completed the microscope
by providing fine adjustment of the sample position with respect to the optical system.
[0103] The fluorescence from cells passing through the channel was analyzed in real time
and a RF pulse was applied to the transducer to sort desired cells with minimal latency.
The photomultiplier tube module measured the intensity of light in the accepted wavelength
range and generated a voltage proportional to the intensity of the incident light.
This voltage was digitized by the data acquisition card (PCIe-7842R, National Instruments
Corp., Austin, TX) and analyzed in real time using the on-board field programmable
gate array to extract the details of the fluorescence peak and generate the sorting
pulse for desired peaks. Instrument settings and plots of the instrument performance
were read out on the associated PC. Here, the sorting pulse was a 5V signal used to
modulate the output of a waveform generator (SMB 100A, Rohde & Schwarz, Munich, Germany)
through its pulse modulation input. The output of the waveform generator was intensified
using a high gain RF amplifier (LZY-22+, Mini-Circuits, Brooklyn, NY). The amplified
RF signal drove the IDT to generate the SAW.
[0104] A custom-made sample holder supported the groove enhanced device. A printed circuit
board (PCB) was connected to the RF amplifier using an MMCX male card edge connector.
The PCB was held in place by fixing it to a mechanical base plate using M3 screws.
Electrical connections from the PCB to the IDT were created, when pogo pins mounted
on the board were pressed into contact with metal pads on the surface of the transducer.
An acrylic spacer milled to 3.7mm and laser cut to match the accommodate the mounting
holes ensured that the pins exerted enough force to hold the IDT in place and make
consistent electrical contact, but not so much force that the substrate cracked under
the stress. Each PDMS device was bonded to the substrate using mechanical force. The
PDMS replica contained three sides of the device's flow channel, while the lithium
niobate substrate formed the bottom of the flow channel. A 6 mm sheet of acrylic was
laser cut to permit fluid connections to pass through the sheet. The acrylic pressed
the PDMS onto the substrate using M2 screws to couple the acrylic layer to the baseplate.
Once assembled, the entire sample holder fit into the microscope stage.
[0105] Characterization experiments. Madin Darby canine kidney (MDCK) and human chronic
myelogenous leukemia (K-562, ATCC, Manassas, VA) cells were harvested prior to each
day's experiments. The MDCKs have fluorescent nuclei, having been stably transfected
with green fluorescent protein fused to a nuclear localization sequence, while the
K-562 cells were stained by adding calcein AM (Life Technologies, Grand Island, NY)
to the cell suspension at a concentration of 1 micro molar and incubated the suspension
at 37 °C for 20 minutes. The cells were re-suspended into injection buffer at between
5 and 10 million cells per ml. The injection buffer was 18% Optiprep (D1556, Sigma-Aldrich
Co. LLC, St. Louis, MO) by volume, 6 U/ml DNAse I (New England Biolabs Inc., Ipwich,
MA), 3 micromolar magnesium chloride and 1X phosphate buffered saline.
[0106] Unless otherwise specified, the testing conditions were applied to a device with
a slanted groove that was 120 micrometers wide, and whose long axis was tilted 60°
from the overall direction of flow. Sheathes of 1X phosphate-buffered saline (PBS,
P3813, Sigma-Aldrich Co. LLC, St. Louis, MO) were used. The total sheath flow rate
was typically 45 ml/h, with a quarter of the flow coming from the sheath inlet closer
to the waste channel and three quarters of the flow from the sheath inlet on the retention
side of the device. The cell phase flow rate was 0.5 ml/h. The frequency of the RF
pulse was usually kept constant at 163.1 MHz, but when the groove width changes, then
the frequency was varied to ensure that the SAW actuation aligned with the groove.
Prior to testing the sorting performance for each distinct condition, control experiments
were run to ensure that cells were not sorted, when the instrument was triggered but
no acoustic wave was applied. Each characterization experiment varied only one element
of the standard conditions at a time, and each condition was tested on three independent
days of experiment. As mentioned previously, fast movies of individual sorting events
were analyzed to determine whether a cell was successfully deflected across the sorting
channel into the retention outlet or not.
[0107] Sorting experiments. As detailed for the characterization experiments, K-562 cells
were harvested from culture just prior to conducting the experiment. To create reference
libraries of cells, the sample of cells were mixed carefully and 10% of the cell suspension
by volume was collected. This fraction of the cells was stained with calcein AM at
1 micromolar for 20 minutes at 37 °C, while the remaining cells remained unstained.
The two fractions were then combined and the cells re-suspended in injection buffer
at the target cell density.
[0108] The cells were sorted using a slanted groove sorting device. A standard nozzle geometry
and an RF pulse with 38.26 dBm of instantaneous power and 100 microsecond duration
at 164.1 MHz was used. The flow rate of the cell suspension was kept constant at 0.5
ml/h. The device was operated with a range of cell densities to create test different
event rates. Over the entire cell density range, the purity from devices operating
at two different sheath flow rates, 45 ml/h and 60 ml/h was measured, and using two
different groove widths, 40 micrometers and 80 micrometers, under the same sorting
conditions. Here, the sheath flow was also 1X PBS. The actual rate of fluorescent
events was measured by the sorting instrument and the projected total event rate was
obtained by dividing this by the measured purity of the initial reference library.
The thresholds for sorting were set to ensure that pulses were only applied when only
a single fluorescent cell was expected to be present in the channel, by ignoring the
lower and upper extremes of fluorescence. In addition, when the sorting rate is high,
the sorting thresholds were further limited to set the sorting rate below 500 events/s,
reducing the chance that the IDT will be damaged irreparably. However, this limit
was somewhat arbitrarily set.
[0109] The fluorescence of the cells recovered from the retention outlet was measured using
a confocal microscope (SP5, Leica Microsystems Inc., Buffalo Grove, IL). In addition
to using calcein to measure the proportion of labelled cells in the recovered sample,
DRAQ5 (Life Technologies, Grand Island, NY) was added at a final concentration of
500 nM to label the DNA of all cells present in each sample. To measure cell viability
after sorting, ethidium homodimer (Life Technologies, Grand Island, NY) was added
to 2 micromolar final concentration and the cells incubated for 20 minutes at 37 °C.
The images were analyzed using a custom Matlab (The Mathworks, Inc., Natick, MA) script
to detect fluorescence in the three separate fluorescence channels. The purity of
the sorted fraction was determined by determining the ratio of cells labeled with
calcein to total number of cells, and the viability was determined as the complement
of the ratio of dead cells to total cells.
[0110] The scope of the invention is defined by the appended claims.